Session A7 Paper #56 Disclaimer—This paper partially fulfills a writing requirement for first year (freshman) engineering students at the University of Pittsburgh Swanson School of Engineering. This paper is a student, not a professional, paper. This paper is based on publicly available information and may not provide complete analyses of all relevant data. If this paper is used for any purpose other than these authors’ partial fulfillment of a writing requirement for first year (freshman) engineering students at the University of Pittsburgh Swanson School of Engineering, the user does so at his or her own risk. NUCLEAR FUSION THROUGH TOKAMAK CONFINEMENT SYSTEMS John Hiller, [email protected], Lora 3:00, Benjamin Page, [email protected], Mahboobin 10:00 Abstract—Nuclear Fusion is an experimental form of energy which involves the heating and confinement of different hydrogen isotopes until they can fuse together and produce energy. Tokamaks are a form of magnetic confinement system originally developed in 1951 by soviet physicists Andrei Sakharov and Igor Tamm. Tokamaks make use of a toroidal, or donut shape, configuration which together with an induced electric field confines the hydrogen plasma used to fuel nuclear fusion into a closed loop. Within a tokamak, the plasma fuel acts as the secondary winding of a transformer, while the primary winding is an external coil. The external coil’s winding induces a current in the plasma and coupled with field coils surrounding the toroidal shape and generates the magnetic field. Tokamaks offer a design for devices which can facilitate nuclear fusion that has the potential for international implementation and that has received a great amount of research. Currently numerous tokamaks have been or are being developed for research purposes, including JET and ITER. Research tokamaks serve as both investigative tools and examples of the potential of fusion power. Although the implementation of tokamaks offering energy on a large enough scale for commercial use is still decades away, they still represent a promising option for the future of nuclear fusion. and fuse the ions together [1]. Thus, the ions fuse and cause a release of energy. Due to the great amount of invested research, the behavior of fusion reactions is well understood and represent a future of harnessable clean energy. As of today, the main challenges remaining with fusion power lie more in the design and construction of commercial fusion reactors, as the conditions required for a fusion reaction are already understood. Although small-scale research reactors, which are present internationally, offer a valuable source of information for the behavior of aspects of fusion reactions, such as the plasma behavior devices, and what will be required for their operation, they are not able to supply energy at levels high enough to be used for any sort of commercial implementation. Fusion vs Fission In a fission reaction, the nucleus of a uranium atom absorbs a neutron causing it to become unstable and break up. This results in the production of additional neutrons which hit more uranium atoms and trigger a chain reaction [2]. Although fusion reactions are much harder to facilitate, they do not involve any form of chain reaction like that which is present in fission. As stated, fusion reactions simply require its plasma fuel to be heated and contained. This means there is no risk of a runaway process in a fusion reaction, making fusion an allaround safer method of harnessing nuclear power. Key Words—ITER, JET, K-DEMO, K-STAR, Magnetic Confinement, Nuclear Fusion, Tokamaks AN INTRODUCTION TO NUCLEAR FUSION The Fuel for Fusion Fusion is the process in which hydrogen atoms fuse together forming helium, and converting matter into energy. When heated to high enough temperatures hydrogen gas is converted into a plasma causing its negatively charged electrons and positively charged atomic nuclei, or ions, to become separate [1]. On earth fusion is impossible under normal circumstances. This is because the repulsive electrostatic forces between ions of separate atoms of hydrogen prevent any collision from occurring. However, if hydrogen atoms experience a high enough temperature increase fusion can become possible. The temperature increase causes the speed of individual ions to become so great that they can overcome the repulsive electrostatic force and move near enough together for the attractive nuclear force to take over Different isotopes of Hydrogen fuel Fusion reactions. Fusion reactions are most easily fueled by deuterium and tritium isotopes, or D-T fuel. D-T fusion reactions release over four times as much energy as uranium fission on a basis of mass [1]. Deuterium is abundant, occurring naturally in seawater. Tritium, although not largely naturally occurring, can be created in a fusion system from lithium, which is present in large quantities on earth [1]. A blanket containing lithium which surrounds the reactors core will absorb Neutrons produced by D-T reactions. This causes the lithium to be transformed into tritium, which will then act to fuel further reactions, and helium. Finally, although D-T reactions can produce a great energy yield fusion has a much lower power 1 University of Pittsburgh Swanson School of Engineering 3/31//17 John Hiller Benjamin Page The plasma’s ions and electrons travel along generated magnetic field lines, but are unable to cross the lines [3]. Magnetic confinement systems are constructed in toroidal, or doughnut shaped, configuration. Toroidal configurations have their magnetic fields curved around them to form closed loops [1]. Also, a superimposed perpendicular field component, or poloidal field, is required for proper confinement. The result is a magnetic field with spiral, or helical, path force lines that confine the plasma. density than fission. This means that fusion reactors will require greater sizes and costs than fission reactors. The use of Tritium as part of the fusion fuel creates a possible issue associated with nuclear fusion. Tritium is weakly radioactive and, although it may not represent a great environmental concern, it can be harmful if brought directly into contact with the human body [1]. Because of this there is interest in the use of Deuterium Deuterium, or D-D reactions, but these would require even greater temperatures and thusly this form of fuel is often only used in small-scale research reactors. Future use of D-D reactions means tritium only represents a temporary problem. However if a large enough safety concern is created, Tritium could still represent a possible delay when nuclear fusion finally begins large scale commercial implementation. An understanding of the fusion fuel allows for a better explanation of the sustainability of nuclear fusion. The components of D-T fuel can be easily found on earth, or created directly inside of a fusion device. Additionally, if D-D fuel is ever achieved on a commercial level, fusion reactions will easily be fueled by an abundant natural resource. The challenge associated with fusion is the construction of a device capable continuous facilitation of fusion reactions. Facilitating Fusion Reactions For a fusion reaction to successfully occur on earth a device must be developed which can heat the D-T fuel to temperatures of the order of 50 million degrees Celsius while also keeping it under intense pressure. This will allow the fuel to be kept dense enough and confined long enough for the hydrogens nuclei to fuse. Fusion research programs work towards achieving what is known as ignition. Ignition is the point at which fusion reactions produce net energy and become self-sustaining, only requiring fresh fuel to be added to continue it [1]. When ignition is finally achieved, the net energy produced is about four times greater than that of a fission reaction. This resulting greater energy yield represents the potential and importance of developing the future of fusion technology. Currently one method of facilitating fusion reactions being studied is magnetic confinement, which makes use of magnetic fields to contain the plasma fuel. FIGURE 1 [4] Simple Diagram of Field Components Figure 1 offers a simple illustration of the toroidal and poloidal field components required in the use of magnetic confinement system. Also included is the resulting helical path which the plasma fuel will be confined along The effectiveness of the toroidal shaped reactor is seen within the helical path the plasma fuel is confined along. The fuel forms a closed loop which travels throughout the torus shape, but remains isolated from the reactor walls. One form of toroidal confinement system which is receiving various international research is the tokamak. MAGNETIC CONFINEMENT SYSTEMS THE TOKAMAK One method of facilitating fusion reactions which has received a heavy amount of research and shown potential for success is using Magnetic Confinement systems. Magnetic confinement systems make use of strong magnetic fields to confine D-T plasma under atmospheres of pressure while it is heated to fusion temperatures [1]. These strong magnetic fields isolate the plasma from air by confining them in a vacuum vessel. The use of magnetic fields to confine plasma are ideal, because of the plasma’s separated electrons and ions. Tokamaks are a form of magnetic confinement system originally developed in 1951 by soviet physicists Andrei Sakharov and Igor Tamm [1]. Tokamaks lack the complexity present in the designing and building of the stellarator, another form of magnetic confinement system [1]. The simpler design has caused tokamaks to become more favored, leading to abundant international research in the form of several small-scale tokamaks. Because of their lack of 2 John Hiller Benjamin Page complexity and the large amount of research invested into them, tokamaks represent what could soon become an accessible method of commercial use of nuclear fusion power. How Tokamaks Work Within a tokamak an external coil, the central solenoid, and the plasma fuel itself act as the respective primary and secondary windings of a transformer [3]. A current is induced in the plasma by a change of current in the central solenoid. This current also provides a portion of the heating required for the plasma to undergo the fusion reaction. The remaining portion of heating required is supplied through high-frequency heating, which makes use of electromagnetic waves of different frequencies. These waves heat the plasma through resonant absorption, meaning energized neutral particles penetrate the plasma and transfer their kinetic energy through collisions with plasma particles [3]. Toroidal and poloidal field coils which surround torus shaped vacuum vessel which isolates the plasma from air generate the confining magnetic field [3]. The toroidal coils are evenly spaced vertically around the vessel and generate the toroidal field and the poloidal coils, which generate the perpendicular field component, are placed horizontally around the toroidal coils [1]. The resulting helical magnetic field generally has a strength of around 5 tesla, about 100,000 times as strong as earth’s magnetic field [3]. The inside of the vacuum vessel is lined with lithium containing blanket modules, which react with the neutrons resulting from fusion reactions [3]. This in turn produces additional tritium to fuel further reactions and causes the neutrons energy to be removed from the vessel and heat a water circuit which produces steam to power the actual electrical generators. Further components include a divertor which removes impurities and Helium resulting from fusion reactors from the vacuum vessel, and a cryostat which keeps the superconducting magnets cooled to their operating temperature of -269 degrees Celsius [3]. FIGURE 2 [4] Diagram of major tokamak components The above diagram offers a look at the configurations of the major tokamak components. Included in the diagram are the toroidal and poloidal coils, their filed components, and the resulting helical magnetic field, as well as the external coil and current induced in the plasma, which correspond to the primary and secondary transformer circuits. The tokamak offers a simple design which makes use of magnetic fields to allow for fusion reactions to be continuously facilitated. Despite the large scale a commercial tokamak will require to produce usable energy, the tokamaks design has continuously been successfully tested by many international research reactors EXAMPLES OF TOKAMAKS Many examples of operational tokamaks, which are built on a small-scale for research purposes, exist internationally today. Additionally, there are certain international efforts being made to develop large-scale research tokamaks, which will act to imitate the operations of commercial tokamaks. Both small-scale and large-scale tokamaks act as valuable resources of information of the behavior of tokamak confinement systems and the possibilities of nuclear fusion. JET the Largest Operating Tokamak The Joint European Torus, or JET, is an operational research tokamak used by more than 40 European laboratories, with 350 scientists and engineers contributing to its operation 3 John Hiller Benjamin Page [4]. JET originally began operation in 1983. As of July, of 2014 a 283-million-euro contract signed between the European Commission and the Culham Centre for Fusion Energy, or CCFE, which secured JET’s operation until 2018. The original purpose of JET was to study the plasma behavior in conditions mimicking those of a commercial fusion reactor. JET is the largest and most powerful tokamak in the world and the only device capable of making use of the D-T plasma fuel which is planned for use in commercial reactors [4]. This is important because, unlike other smaller research tokamaks which make use of D-D fuel, JET allows for the closest possible look at the plasma behaviors in future D-T devices. However, today its purpose is to act as preparation for the ITER tokamak, another research tokamak which has not yet been constructed. Throughout the years of its operation, JET has received upgrades to make it more like ITER so that it can better prepare for ITER’s operation. One important upgrade was to equip JET’s vacuum vessel’s inner wall with the same materials which will be used in ITER’s construction, beryllium and tungsten [4]. The new wall, in association with upgraded heating power, will allow for plasma scenarios closely resembling those expected in ITER. JET experiments have already allowed for the decision to be made to have ITER operate with a fully tungsten divertor, which will reduce investment costs. Another important task JET has been set to is ELM mitigation [4]. ELMs, or Edge Localized Modes, are short plasma outbursts which cause large heat and particle loads to be thrust onto the vacuum vessel walls. Within devices as powerful as ITER, ELMs represent a large risk for the vessel wall, because of this JET has been tasked with prediction and mitigation of these events. Both JETs early and more recent operation purposes have been very important for the future of nuclear fusion power. Before JET was tasked with aiding in the preparation of ITER it offered a valuable resource for understanding the behavior of the D-T plasma which will be used in large-scale tokamaks such as ITER. However, after it began to be upgraded to more resemble ITER, JET became even more important for the future development of commercial nuclear fusion. Because ITER will be designed on a much larger, commercial mimicking scale, having JET offer a possible preview of how ITER will behave will likely allow for ITERs operators to be better prepared following ITERs construction. Additionally, as it continues its operation, JET could continue to allow for a better understanding of how ITER must be constructed to be most successful, possibly allowing for further reduction of investment costs, and what can be expected in ITERs operation. ITER, international thermonuclear experimental reactor, is a research tokamak being developed through a 35nation collaboration. ITER’s purpose is to prove the feasibility of a tokamak system on a scale large enough for commercial implementation [5]. The idea for ITER first began in 1985 and, since then, has received design contributions form thousands of engineers and scientists. ITER will act to bridge the gap between preceding small-scale research tokamak devices and future large-scale commercial tokamak devices. ITER’s purpose is to achieve net energy production, maintain fusion for long periods of time, and test the tokamak designs when producing energy necessary for commercial production [5]. ITER will have ten times the plasma volume as JET, the current largest operating tokamak. Because the amount of fusion energy is a direct result of the amount of fusion reactions taking place within a fusion reactor, this increased volume will allow for the large-scale fusion reactions needed for ITERs goals. Currently the largest amount of fusion power ever produced on earth is 16 megawatts [5]. JET achieved this output in 1997, and required a total power input of 24 megawatts. ITER is designed to produce a record breaking 500 megawatts of fusion and at the input cost of only 50 megawatts of power. Although ITER will not be designed to capture the produced energy as electricity it will be the first fusion experiment to produce a net energy gain. ITER is also expected to achieve a so called “burning plasma,” in which the heat of a fusion reaction is confined within the plasma fuel. This will allow for longer sustained reactions which have never been achieved. ITER will also act as an experiment for the capabilities of in-vessel tritium breeding [5]. This is important to the future of fusion technology because of the lack of naturally occurring tritium. Successful tritium breeding will allow for proof of a continuously sustainable fusion fuel for future commercial fusion devices. Finally, ITER will be demonstrative of the general operation and safety of commercial scale fusion devices. ITER will also act to demonstrate the negligible environmental consequences present in large scale fusion fuel synthesis and fusion reactions. ITER represents a large step in the direction of commercial nuclear fusion. Although still experimental, ITER will produce energy which will dwarf levels present in previous research tokamaks and, more importantly, this energy will heavily outweigh the energy input into the device. ITER is not expected to have its first plasma prepared until December of 2025, and D-T operations are projected to begin in 2035 [5]. ITER, JETs Successor K-DEMO a Step for Tokamaks after ITER 4 John Hiller Benjamin Page resource in ensuring the safety of operation when faced large amounts of runaway currents, such as those expected in ITERs operation. This will likely allow for more reliability in future tokamak operation. Following a Korean fusion energy development promotion law, or FEDPL, enacted in 2007 a design for a Korean fusion demonstration reactor, or K-DEMO, was initiated in 2012 [6]. K-DEMOs construction is expected by 2037 with a scale comparable to that of ITER. However, a special development plan may cause K-DEMO to represent the commercial next step for Tokamaks. A special concept which has been proposed as a possibility for K-DEMO is a development plan over two phases. Its first phase will resemble purposes like that of ITER. K-DEMO will design a net energy gain and sustained in-vessel tritium breeding, as well as acting as a component test facility. During its second phase, in-vessel components will be upgraded. This upgrade will allow K-DEMO to show not only net energy gain, but also net electric generation of about 500 MW. Unlike ITER, K-DEMO will work to harness its energy gain as electric power, rather than just demonstrating large scale net energy. Therefore K-DEMO can be viewed as a likely next step for commercial tokamaks. IMPACTS OF TOKAMAKS Despite the research heavily invested into the safety and reliability of tokamaks, possible negative impacts are still present in future commercial use. One such impact lies in the use of D-T plasma fuel, specifically in the tritium isotope. Although tritium does not represent a heavy environmental concern, it is weakly radioactive. Due to it being an isotope of hydrogen, it can enter the human body and cause health concerns [8]. Because an increase in local levels of tritium have been observed in association with nuclear devices, this could represent a need for greater safety to be applied to tokamaks before international commercial implementation. Another issue associated with the tokamak has to do with the producing of certain components and the associated price. A tokamaks major price contributions have to do with its toroidal and poloidal field coils, and its use of an external coil. Tokamak filed coils are much larger than those associated with other magnetic confinement systems, which means when they must be built directly on the devices construction site, or shipped in through unconventional means [9]. Also, the external coil which the tokamak makes use is not present in other magnetic confinement systems. This means that the tokamaks encounter an additional price point when compared to alternative confinement systems to achieve a simpler and easier to implement design. K-STAR and ECRH The Korea superconducting tokamak advanced research device, or K-STAR, is a small-scale research tokamak which has acted to investigate the behavior of relativistic runaway electrons during electron cyclotron resonance heating, or ECRH [7]. Relativistic runaway electrons generated within tokamaks can cause severe damage through collisions with vacuum vessel walls. Because ITER is expected to experience a large amount of runaway currents research into runaway electrons is of great importance. Regularly, the growth rate of runaway electrons can be diminished by increases in electron density [7]. However, the density required for a large-scale tokamak such as ITER may not be accomplishable and, even if it were, it may adversely affect the vacuum vessel. K-STAR therefore underwent experimentation of runaway electron growth rate decrease using ECRH discharges. K-STAR observed the electron behavior through brief usage of the hard x-ray, or HXR, monitor system [7]. Through its experimentation, KSTAR found that ECRH discharges could lower runaway electron discharge rates, but also experienced an unexpected phenomenon. It was found that under certain plasma conditions superthermal electron generation occurred during ECRH. This meant that tokamaks using ECRH must take care to observe plasma conditions when employing ECRH based suppression. K-STARs research is important because of the service it provided for ITER and future commercial tokamaks. Large scale tokamaks have been provided with a valuable THE FUTURE FOR TOKAMAKS AND NUCLEAR FUSION Despite the progress being made in the research of tokamaks and their future implementation, commercial use of nuclear fusion is still a long way off. Still, many strides toward commercial tokamaks have been made and through research projects like ITER the potential for nuclear power can be presented on an international level. Additionally, although the implementation and continued operation of tokamaks will largely be a job for future generations, it can be seen through projects like K-DEMO that commercial nuclear fusion has not simply been disregarded as solely a technology reserved for the future. Through the combined efforts of scientists and engineers of today and tomorrow, the use of large scale nuclear fusion can be achieved and implemented on an international level. SOURCES 5 John Hiller Benjamin Page [1] “Nuclear Fusion Power.” world-nuclear.org. 12.20.2016 Accessed 1.8.2017http://www.world-nuclear.org/informationlibrary/current-and-future-generation/nuclear-fusionpower.aspx [2] “How do fission and fusion reactions compare?” eurofusion.org. Accessed 2.21.2017 https://www.eurofusion.org/faq/how-do-fission-and-fusion-reactions-compare/ [3] Fusion Research: An Energy Option for Europe’s Future. Luxembourg: Office for Official Publications of the European Communities, 2007 [4] “JET” euro-fusion.org Accessed 1.11.2017 https://www.euro-fusion.org/jet/ [5] “What is ITER?” iter.org. Accessed 1.9.2017 http://www.iter.org/proj/inafewlines [6] K. Kim, K. Im, H.C. Kim, S. Oh, J.S. Park, S. Kwon, Y.S. Lee, J.H. Yeom, C. Lee, G-S. Lee, G. Neilson, C. Kessel, T. Brown, P. Titus, D. Mikkelsen and Y. Zhai Design Concept for K-DEMO for near-term implementation IOP publishing 4.11.2015 accessed 1.27.2017 http://iopscience.iop.org/article/10.1088/00295515/55/5/053027/pdf [7] C. S. Kang, S.G. Lee. “Investigation of relativistic runaway electrons in electron cyclotron resonance heating discharges on Korea Superconducting Tokamak Advanced Research” Publish July 2014 Accessed 1.26.2017 http://aip.scitation.org/doi/full/10.1063/1.4890461 [8] “Tritium and the Environment” 8.9.2012 Accessed 1.11.2017 http://www.irsn.fr/EN/Research/publicationsdocumentation/radionuclidessheets/environment/Pages/Tritium-environment.aspx [8] R. Siemon, I. Lindemuth, K. Schoenberg. “Why Magnetized Target Fusion Offers A Low-Cost Development Path for Fusion Energy” 11.12.1997 Accessed 1.11.2017 http://fusionenergy.lanl.gov/Documents/MTF/Why_MTF/Wh y-MTF-Comments.html ACKNOWLEDGMENTS The authors would like to acknowledge their fellow Forbes hall floor 4 residents who, through their concurrent hard work helped to motivate us in writing our paper. 6
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